RING LASER GYROSCOPE LINEARIZATION SYSTEM

摘要

1321208 Lasers NORTH AMERICAN ROCKWELL CORP 25 Feb 1972 [19 April 1971] 8898/72 Heading G4H [Also in Division H1] In a ring laser which exhibits a non-linear characteristic in regions just above its lock-in rotation rate, the cosine of the ring output beat frequency is used to control one of the laser resonator mirrors and the sine of the output is used to derive a corrected signal which represents the true rotation rate of the laser. In Fig. 1 the apparent rotation rate given by a ring laser is plotted against its actual rotation rate Q. As is usual there is a minimum rotation rate Q L below which the laser gives zero output, the present invention does not affect this. There is also a region 7 where there is an output from the laser, but its value is incorrect. The ring laser shown in Fig. 3 is controlled so that its output may be corrected to give the true rotation rate shown at 6 in Fig. 1. In Fig. 3 one output beam from the laser 12 passes to photodetector 1 via a beam splitter 18, while the other output beam is first reflected by a vibratable mirror 11 before reaching the beam splitter. The combined beams are incident on the photodetector 1, and produce a sine function signal as shown in Fig. 4. This sine function is integrated to give a cosine signal at 2 in Fig. 3, and is passed to a counter 3. The counter is of the type which adds when the cosine signal is +ve and subtracts when it is -ve; the counter also receives a clock signal, so that its output is representative of the difference in the length of time of + ve and - ve half cycles of the cosine signal. The output is passed via D to A converter and a transfer network 5 to a piezoelectric mirror mount 24, the motion of the mirror being such as to minimize the difference between the length of the half cycles of the cosine signal. A sine signal is shown in Fig. 4, and represents the output from the photodetector when the cosine half cycles have been made equal in time. The sine signal is fed to a counter 7 which works in the same manner as the previous counter 3 so as to give a signal representing T 1 -T 2 on Fig. 4. It is also fed to a counter 8 which produces a signal representing T 1 +T 2 ; the two signals are passed to a ratio multiplier 9 to give a signal (#)/(2).(T 1 -T 2 )/(T 1 +T 2 ). The cosecant of this is generated at 16 and passed to a linear accumulator 17. The output from the accumulator forms the corrected output of the ring laser shown at 6 in Fig. 1.